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Atmosphere-Ocean Interaction

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Presentation on theme: "Atmosphere-Ocean Interaction"— Presentation transcript:

1 Atmosphere-Ocean Interaction

2 Upcoming Schedule Monday, March 17: finish Chapter 10 + office hours
Wednesday, March 19: Second midterm exam. The exam will cover Chapters 6, 7, 8, 9 and 10. Closed book No textbooks, calculators or cheatsheets. Alternate (anti-social) seating Bring a picture ID to the exam. Remember to: Write the 5-digit test code in lines 76-80 Write your name on the exam sheet and sign it Turn in both the exam sheet and the answer sheet. Friday, March 21: begin Chapter 11.

3 The Single Cell Model This is a very simplified model based on the following three assumptions: The Earth’s surface is uniformly covered with water (no differential heating of the land and the oceans) The sun is always directly over the equator (no seasonal variations of the winds). The Earth does not rotate. No Coriolis effect. The only active force is the pressure gradient force.

4 The Three Cell Model Keep two of the assumptions, relax the third:
The Earth is covered with a continuous ocean The sun is always directly over the equator The Earth rotates -> Coriolis force!

5 Observing global winds
Intertropical convergence zone Observing global winds from space

6 Winds and pressure in the real world
Semi-permanent highs and lows: persist throughout the year, correspond to converging/diverging upper air masses. Bermuda, Pacific highs; Icelandic, Aleutian lows Seasonal highs and lows (continents heat/cool faster) Winter: Siberian high, Canadian high Summer (thermal lows): Southwest US, Iran January July Subtropical highs Subtropical highs

7 Does it work? Yes: semi-permanent highs and lows: persist throughout the year No: seasonal highs and lows (continents heat/cool faster) No: seasonal shifts N-S (today) No: winds aloft in mid latitudes January July Subtropical highs Subtropical highs

8 Effect on the local climate
During summer, the Pacific high moves north near the CA coast, and the Bermuda high moves closer to the SE coast. CA: dry summers GA: wet summers

9 Seasonal Effects on the Global Circulation.
January The three cell model neglects the Earth’s tilt The tilt would cause seasonal N-S shifts Bright white colors correspond to stronger winds. The winds are stronger in the winter. The wind system shifts slightly north-south during the year (think of bird migration) July

10 The General Circulation and Precipitation Paterns
Converging surface flows: Low surface pressure Uprising air Heavy precipitation Diverging surface flows: High surface pressure Sinking air Dry climate Seasonal variations of the climate. Example: Timbo, Guinea (Chapter 17). Timbo

11 Example: Tropical wet-and-dry climate (Aw)
Timbo (Guinea) Wet summer season Dry season (Dec-Feb): hot, desert-like conditions Grassland savanna

12 Winds and Pressure Systems Aloft
The wind system aloft differs from the surface wind system. It is close to a geostrophic flow. There is no significant friction with the ground. The three cell model does not work that well in the middle latitudes. The winds aloft are stronger than on the ground. In the winter the gradients are bigger -> the winds are stronger. July January

13 Winds Aloft Warm air above the equator and cold air above the polar regions Higher pressure at the equator, lower pressure both to the north and to the south of the equator The pressure gradient force is towards the poles, sets the air in motion The Coriolis force NH: to the right SH: to the left The wind turns right in the NH and left in the SH, becomes parallel to the isobars Westerly winds aloft in both the NH and SH. Easterly winds at the surface in both the NH and SH.

14 Jet Streams Swiftly flowing air currents aloft Tropopause jets
Subtropical: 13km high, 30N Polar: 10km high, 60N Strong westward winds Meandering pattern They result from strong temperature gradients at those latitudes (hence strong PG forces)

15 Tropopause jet streams
Discontinuous. Position varies daily. May merge or split (northern and southern branches) Meandering pattern: may flow to the north or south Important for the global heat redistribution Affect local weather conditions

16 Atmosphere-Ocean Interaction
The surface of the Earth impacts the air motion through the friction force. Newton’s III law: for every action there is a reaction. The atmosphere exerts a friction (drag) force on the surface of the Earth. The prevailing surface winds drive the surface currents in the oceans. Variations in the surface temperature of the ocean impacts the atmospheric T as well as amount of the water vapor in the atmosphere.

17 Major ocean currents Gyres: circular whirls of ocean currents
25-40 deg angle b/n wind and current Clockwise in the North Pacific and Atlantic Counterclockwise in the South Pacific and Atlantic

18 Ekman Spiral The surface winds drive the surface currents.
The friction force acting on the ocean surface is in the direction of the wind. The Coriolis force deflects the current to the right (NH). Each layer of water drags the water layer below, and the Coriolis force pushes the moving water below to the right. The direction of the ocean current changes with depth. The net mass transport within the first 100 m is perpendicular to the wind direction.

19 Upwelling of the Ocean Water
Winds plowing along the coastal line result in a net surface current perpendicular to the wind and away from the coast. The warm surface water is replaced by an upwelling deep cold water. Water upwelling explains the low water temperatures along the California coast.

20 Surface Water Temperature Along California’s Coast
The low water temperatures result in low saturation vapor pressure over the ocean. Recall the advection fog example from Chapter 5 As the air moves over the land the air warms up and results in low relative humidity. The summer is very dry.


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